{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:4CIEKCRVRTVMZ47FQCUQPA6WST","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"98c298ee668d60490327903d294d0edfaba604fdbaf720bbbd1b80b69f793918","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-20T10:16:42Z","title_canon_sha256":"39051deef3692346affa2b960942ccf1a25304f6c058f75eba233ea6c42ee18d"},"schema_version":"1.0","source":{"id":"2409.13372","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.13372","created_at":"2026-07-05T09:09:34Z"},{"alias_kind":"arxiv_version","alias_value":"2409.13372v1","created_at":"2026-07-05T09:09:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.13372","created_at":"2026-07-05T09:09:34Z"},{"alias_kind":"pith_short_12","alias_value":"4CIEKCRVRTVM","created_at":"2026-07-05T09:09:34Z"},{"alias_kind":"pith_short_16","alias_value":"4CIEKCRVRTVMZ47F","created_at":"2026-07-05T09:09:34Z"},{"alias_kind":"pith_short_8","alias_value":"4CIEKCRV","created_at":"2026-07-05T09:09:34Z"}],"graph_snapshots":[{"event_id":"sha256:48a247364399d439eca6d9ee58fdd4680ea5dbc56ee1ccf73e75be75d92845cf","target":"graph","created_at":"2026-07-05T09:09:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2409.13372/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Non-Hermitian systems, going beyond conventional Hermitian systems, have brought in intriguing concepts such as exceptional points and complex spectral topology as well as exotic phenomena such as non-Hermitian skin effects (NHSEs). However, previous studies on non-Hermitian systems predominantly focus on the properties of eigenstates, with rather limited discussions on non-Hermitian dynamic phenomena. Here, inspired by the celebrated success of the parity-time symmetry in non-Hermitian physics, we theoretically study a one-dimensional non-Hermitian system with glide-time reversal (GT) symmetr","authors_text":"Jian-Hua Jiang, Li-Wei Wang","cross_cats":["cond-mat.mtrl-sci","physics.optics"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-20T10:16:42Z","title":"Non-Hermitian glide-time symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.13372","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:81ff39b39a4b5c0f6e0679a3df7140195002c6a3ed82a8cf29f8de0c37094ae6","target":"record","created_at":"2026-07-05T09:09:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"98c298ee668d60490327903d294d0edfaba604fdbaf720bbbd1b80b69f793918","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-20T10:16:42Z","title_canon_sha256":"39051deef3692346affa2b960942ccf1a25304f6c058f75eba233ea6c42ee18d"},"schema_version":"1.0","source":{"id":"2409.13372","kind":"arxiv","version":1}},"canonical_sha256":"e090450a358ceaccf3e580a90783d694f677df161d1119b375220a21d7791f59","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e090450a358ceaccf3e580a90783d694f677df161d1119b375220a21d7791f59","first_computed_at":"2026-07-05T09:09:34.153864Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:09:34.153864Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R/BT5TMVynCwdSYZjFvglG9ZOB9M0ekYi4U57iH5Ts+XiKc98BmoYTgUNwy5MmQ3oAjVJJkNOiyE0PB0w2xiCg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:09:34.154411Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.13372","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:81ff39b39a4b5c0f6e0679a3df7140195002c6a3ed82a8cf29f8de0c37094ae6","sha256:48a247364399d439eca6d9ee58fdd4680ea5dbc56ee1ccf73e75be75d92845cf"],"state_sha256":"8ee62c85ab319fcc8d45517d5546f261acc06c66963c7159f40e03de44547c9a"}